Gravitational-wave transient detection and multi-messenger

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Gravitational-wave transient
detection and multi-messenger
astrophysics
Ray
y Frey,
y, Universityy of Oregon
g
for the
LIGO
GO Scientific
Sc e t c Collaboration
Co abo at o
and the Virgo Collaboration
LIGO-G1000515
LIGO
G1000515
• Introduction – overview and status of LIGO and Virgo
• Observational results
• A new astronomyy with advanced GW detectors
G1000515
19July2010
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1
Required GW Sensitivity
for Detection
• GW emission requires time varying
quadrupole moment of mass distribution
distribution,
→ gravitational-wave strain, h = δL/ L, is
the analog of the radiation field E in E&M
• Strain estimate:
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19July2010
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2
GW Interferometer principle
•
•
•
•
•
Michelson interferometer with Fabry-Perot cavity arms.
Long baseline: 4 km ( h = δL/ L ) - For h ≈10
10-21, L ≈ 1 km, then δL ≈ 10-18 m
Fabry-Perot Cavity storage time ∼1 ms (∼100 bounces)
Power recycling (x30)
Noise estimate:
5W
10 kW
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Global network of interferometers
LIGO
GEO 600m
4 km & 2 km
VIRGO 3 km
TAMA 300m
→ LCGT !
LSC:
LIGO+GEO
AIGO- R&D
LIGO
4 km
→ “LIGO
A t li ” ?
Australia”
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4
S5/VSR1 sensitivity
2007
LIGO Run S5:
2005-07
Ran at design
sensitivity for
initial LIGO
Virgo Run VSR1:
2007
Data sharing
g with
LIGO/GEO
LIGO S5
2006
S6
2007
Virgo VS R1
2008
G1000515
2009
R2
Adv LIGO
2010
19July2010
R3
2011
TeVpa, Paris
2012
2013
2014
2015
Adv Virgo
5
The LIGO-Virgo network:
sky coverage
LIGO
O Hanford
averrage antenn
na factor
h(t) = Fx hx(t) + F+ h+(t)
Virg
go
ave
erage anten
nna factor
F+ ⊕ Fx
+ GRBs in S5/VSR1
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GW signals classification
unmodeled
matched
filter
Short duration
Long duration
Burst search
Stochastic search
Inspiral search
CW search
Credit: NASA/CXC/ASU/J. Hester et al.
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S5/VSR1 sensitivity to
compact
p
binary
y coalescence
• NS-NS, NS-BH, BH-BH
• Efficient GW radiators: ~10-2 Mc2
• Matched filter analysis for low-mass inspirals
(horizon=
distance to
optimally oriented
and located
binary which
gives SNR=8 in
one detector)
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S5/VSR1 sensitivity to
GW Bursts
• short (< 1s) transients
• unmodeled waveforms
• CCSNe, GRBs, SGRs, …
t (ms)
EGW ≈
π 2c 3
G
2
D 2 f 02 hrss
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LIGO-Virgo Search Results
• No GW detections yet
• However,
H
b
beginning
i i tto make
k astrophysically
t h i ll iinteresting
t
ti lilimits
it
ƒ This talk: Astrophysically targeted transient searches (GRBs, SGRs)
ƒ Others:
• Crab pulsar spindown limit (ApJ 683 (2008) 45 )
• cosmic GW background limit < BBN (Nature 460 (2009) 990 )
• Era of advanced GW detectors is approaching (>2014) in which we
expect GW detections will become frequent (more on this later)
• To take advantage of this opportunity, we have developed a suite of
multi-messenger
lti
pathways
th
to
t fully
f ll explore
l
th
the science
i
(thi talk)
(this
t lk)
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10
Multi-messenger astronomy
with GWs
EM , neutrinos
External
Triggers
Follow
Ups
GW
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Multi-messenger astronomy
with GWs
•
•
•
•
•
•
G1000515
Detection confidence
Event time
Sky position
Improved search sensitivity
Redshift
g
information
Progenitor
19July2010
TeVpa, Paris
12
Multi-messenger astronomy
with GWs – Status
• Externally triggered searches – gamma, X-rays (Swift, Fermi, IPN)
ƒ GRBs
GRB
ƒ SGRs
• Externally triggered searches – neutrinos
ƒ High-energy neutrinos (Ice Cube, ANTARES, …)
• GRBs, ?
ƒ Low-energy neutrinos (Super-K, LVD, Borexino,…)
• Core-collapse supernovae
• Electromagnetic follow-ups
follow ups of GW triggers
ƒ Requires fast (~10 min) id and distribution of LIGO-Virgo trigger (for S6)
• ~few degree resolution with LIGO-Virgo network
ƒ Swift ToO – XRT
ƒ Wide-angle optical telescopes (SkyMapper, TAROT, Quest, …)
ƒ Radio
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Multi-messenger astronomy
with GWs – Status
• Externally triggered searches – gamma, X-rays (Swift, Fermi, IPN)
ƒ GRBs
GRB
Past and ongoing
searches
ƒ SGRs
• Externally triggered searches – neutrinos
ƒ High-energy neutrinos (Ice Cube, Antares, …)
• GRBs, ?
ƒ Low-energy neutrinos (Super-K, LVD, Borexino,…)
• Core-collapse supernovae
• Electromagnetic follow-ups
follow ups of GW triggers
ƒ Requires fast (~10 min) id and distribution of LIGO-Virgo trigger (for S6)
• ~few degree resolution with LIGO-Virgo network
ƒ Swift ToO – XRT
ƒ Wide-angle optical telescopes (SkyMapper, TAROT, Quest, … )
ƒ Radio
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Gamma-ray Bursts and GWs
Long duration GRBs
Long-duration
BATSE
• Associated with core-collapse of
massive stars (“hypernovae”)
GSFC
Both progenitor models would
also give GW emission
Short-duration GRBs
• Associated with binary mergers
(NS NS NS
(NS-NS,
NS-BH)
BH)
• Mergers are efficient GW radiators
EGW ~ 10-2 Mc2
• Massive core collapse – unknown, but
expected to be less efficient
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GRB 070201
• GRB 070201 – a short-duration
gamma ray burst with position
gamma-ray
consistent with M31 (Andromeda),
0.8 Mpc away.
• Such a nearby GRB would have
easily been observed by LIGO if due
to a binary merger
• This hypothesis ruled out at ~99% CL
Revised error box
M
Mazets
et al.,
l A
ApJ
J 680
680, 545
4
• Most likely: SGR in M31 (Eiso~1045
erg)
• Astrophys. J. 681 (2008) 1419
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GRB 070201 (contd)
Binary coalescence exclusion:
Also searched for unmodeled bursts:
Unable to exclude SGR from M31
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Search for GWs from SGRs
• Soft Gamma Repeaters are thought to be
magnetars – highly magnetized neutron stars
• Can emit occasional EM flares (~1042 erg),
giant flares (~1046 erg), or flare “storms”
• Flare mechanism (crust cracking) would
excite vibrational modes → GWs
General idea: Look for GW in
coincidence with flares
+ flare
◊ giant flare
∗
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storm
18
SGRs (contd)
• Search for long-lived quasiperiodic GWs after giant flare SGR 1806-20
ƒ GW energy limits are comparable to total EM energy emission
ƒ
PRD 76 (2007) 062003 (LSC)
• Search for GW bursts at times of 190 flares from 1806-20, 1900+14
ƒ Excess power search for neutron star f-modes (~1.5–3 kHz)
and
arbitrary lower-frequency bursts
ƒ GW energy limits as low as few × 1045 erg; PRL 101 (2008) 21110
• Stack GW signal power from each flare in 2006 SGR 1900+14 “storm”:
Swift, SGR1900+14 storm
30 s
0
ƒ GW energy limit
li i few
f
× 1045 erg; ApJ
A J 701
01 (2009) L68
L68.
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Advanced GW detectors
LIGO S5
2006
S6
2007
Virgo VS R1
2008
2009
R2
GEO HF
2010
R3
2011
2012
2013
Adv LIGO
2014
2015
Adv Virgo
Install Advanced LIGO
Advanced LIGO and Virgo
• Major upgrades
ƒ Lasers
Lasers, optics
optics, suspensions
ƒ Limited by Quantum noise
• 10x better sensitivity
• 1000x bigger search volume
Some elements of advanced
detectors implemented
already in S6 and VSR3
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Multi-messenger astronomy
with GWs – current developments
• Externally triggered searches – gamma, X-rays (Swift, Fermi, IPN)
ƒ GRBs
GRB
ƒ SGRs
• Externally triggered searches – neutrinos
ƒ High-energy neutrinos (IceCube, ANTARES, …)
• GRBs, ?
ƒ Low-energy neutrinos (Super-K, LVD, Borexino,…)
• Core-collapse supernovae
• Electromagnetic follow-ups
follow ups of GW triggers
ƒ Requires fast (~10 min) id and distribution of LIGO-Virgo trigger (for S6)
• ~few degree resolution with LIGO-Virgo network
ƒ Swift ToO – XRT
ƒ Wide-angle optical telescopes (SkyMapper, TAROT, Quest, …)
ƒ Radio
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19July2010
TeVpa, Paris
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High-energy neutrinos + GW
• High-energy neutrinos
possible from GRBs:
baryons accelerated
in relativistic shocks
ƒ Long GRBs
ƒ Short GRBs
ƒ Failed GRBs
ƒ Low-L GRBs
y
• Joint data analysis
planned: LIGO-Virgo
+ IceCube, ANTARES
(e.g.
(e
g Y
Y. Aso
Aso, et al CQG 25
(2008) 114039 )
See Poster by B. Bouhou
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Multi-messenger astronomy
with GWs – current developments
• Externally triggered searches – gamma, X-rays (Swift, Fermi, IPN)
ƒ GRBs
GRB
ƒ SGRs
• Externally triggered searches – neutrinos
ƒ High-energy neutrinos (Ice Cube, ANTARES, …)
• GRBs, ?
ƒ Low-energy neutrinos (Super-K, LVD, Borexino,…)
• Core-collapse supernovae
• Electromagnetic follow-ups
follow ups of GW triggers
ƒ Requires fast (~10 min) id and distribution of LIGO-Virgo trigger (for S6)
• ~few degree resolution with LIGO-Virgo network
ƒ Swift ToO – XRT
ƒ Wide-angle optical telescopes (SkyMapper, TAROT, Quest, …)
ƒ Radio
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TeVpa, Paris
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Core-collapse supernovae
• Classic multi-messenger astronomical
events:
ƒ Gravitational Waves (prompt)
ƒ Neutrinos (prompt, 10s of MeV, 3 flavors)
ƒ Electromagnetic (delayed)
• Optical (EM) signature:
ƒ may be obscured (eg SN 2008iz in M82 missed in optical)
ƒ unable to determine time of bounce to better
than ~ day
• Neutrinos and GWs directly probe physics
of core collapse
ƒ Signatures separated by < seconds
ƒ A tight coincidence window can be used to
establish a correlation
ƒ Sensitivity range of current GW and neutrino
detectors similar
C. D. Ott, A. Burrows, L. Dessart, and E.
Livne. Astrophys. J., 685, 1069, 2008.
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Core-collapse SNe (contd)
• Classic core bounce GW burst
• Perhaps: acoustic pulsations of
proto-neutron star
A. Burrows, E. Livne, L. Dessart, C. D. Ott, and
J. Murphy. Astrophys. J., 655, 416, 2007.
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CCSNe (contd)
• Neutrinos:
ƒ Super-K: ~104 detected neutrinos for galactic SN
ƒ ~1
1 ffor M31
ƒ Next generation (larger) detectors proposed
g agreements
g
for jjoint GW-neutrino
• Currentlyy pursuing
searches
• GW range very uncertain (need detections to understand
the physics!)
• Comparable range for aLIGO/AdV and Super-K (local
group) with weak signals for extragalactic SNe –
coincidence helpful
f
(I. Leonor et al CQG 27 (2009) 084019 )
• Rate: 5 Mpc sensitive range gives
~1 CCSN / 2 y (Ando 2005)
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Multi-messenger astronomy
with GWs – current developments
• Externally triggered searches – gamma, X-rays (Swift, Fermi, IPN)
ƒ GRBs
GRB
ƒ SGRs
• Externally triggered searches – neutrinos
ƒ High-energy neutrinos (Ice Cube, Antares, …)
• GRBs, ?
ƒ Low-energy neutrinos (Super-K, LVD, Borexino,…)
• Core-collapse supernovae
• Electromagnetic follow-ups
follow ups of GW triggers
ƒ Requires fast (~10 min) id and distribution of LIGO-Virgo trigger (for S6)
• ~few degree resolution with LIGO-Virgo network
ƒ Swift ToO – XRT
ƒ Wide-angle optical telescopes (SkyMapper, TAROT, Quest, …)
ƒ Radio
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EM Followups
• First attempts with LIGO-Virgo network Dec, 2009
p
Aug-Sept
g
p 2010
• More expected
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Advanced LIGO/Virgo reach
(example)
NS-NS coalescence reach
BNS sources ∼ Dn
n = 2.7 → 3
D ~ 50 M
Mpc, iinitial
iti l
LIGO/Virgo
p , Adv
~ 500 Mpc,
LIGO/Virgo
Advanced detectors
reach includes
millions of large
galaxies and
hundreds of superclusters
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Binary coalescence
expected rates
arXiv: 1003.2480 (LSC, Virgo)
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GWs, GRBs, Cosmology
• Advanced LIGO/Virgo is sensitive to coalescing NS and/or BH binaries
to distances which are cosmologically relevant.
• The detected waveform is a function of many quantities, including:
• A sample of short GRBs with measured redshifts allow extraction of
Di t
Distance
(DL) independent
i d
d t off EM di
distance
t
lladder
dd (based
(b
d only
l on GR)
ƒ e.g. Dalal et al, PRD 74 (2006) 063006: measure Ho to 2% in a year of
Advanced LIGO data (too optimistic?)
• Sky position ( θ, φ) and beaming constraint ( ι )
improve measurement of DL
ƒ Nissanke
Ni
k ett al,l arXiv:0904:1017
Xi 0904 1017
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Summary
• LIGO and Virgo have accumulated substantial data sets at the
design sensitivity of the initial detectors (runs S5 and VSR1)
ƒ No detections yet, but starting to make interesting statements:
• GRBs, SGRs (and others)
• Current data taking and analysis: Runs S6/VSR2
• Advanced LIGO and Virgo are being constructed
ƒ x10
10 b
better sensitivity;
ii i
x1000
1000 llarger volume
l
ffor sources
ƒ Science turn on ~2015
routine → GW science & astronomy
• Expect detections to become “routine”
ƒ GWs can provide unique information toward understanding the
astrophysics underlying transient sources
• To fully exploit this science, a suite of multi-messenger techniques
have been developed (EM external triggers), while others are now
being
g developed
p and tried ((neutrinos,, EM follow-ups)
p )
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Antenna Pattern
GWs are transverse, with x and + polarizations: hx(t) , h+(t)
“×” polarization
Detector
response
“+” polarization
RMS sensitivity
h(t) = Fx hx(t) + F+ h+(t)
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What Limits Sensitivity
of the Interferometers?
•
Seismic
S
i i noise
i & vibration
ib i
limit at low frequencies
•
Thermal noise of
suspensions and test
masses
•
Quantum nature of light
g
(Shot Noise) limits at high
frequencies
•
Limitations of facilities much
lower
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Science runs and sensitivity
Run
S1
# days
17
Sept ‘02
S2
59
Feb 03-Apr 03
S3
70
Nov 03-Jan 04
S4
30
Feb- March 05
S5
N 05 – Sep
Nov
S 07
2y
(1y
(1
coincident)
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Test Masses
Fused Silica, 10 kg, 25 cm diameter
and 10 cm thick
Polished to λ/1000 (1 nm)
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Length readout and control
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Coalescing Compact Binaries
NS-NS, BH-BH, (BH-NS) binary systems
Matched filter
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Template-less
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Matched filter
38
Numerical relativity
NS-NS, BH-BH, (BH-NS) binary systems
Development of a numerically
stable formalism
formalism…
F. Pretorius, PRL 95 (2005)
X
BH-BH, 10:1 mass ratio, arXiv:0811.3952
LSC+theory “NINJA”: arXiv:0901.4399
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Baker, et al 2008 PRD 78 044046
39
Advanced LIGO
SILICA
180 W
PRM
BS
ITM
ETM
SRM
PD
830 kW
Power Recycling Mirror
Beam Splitter
Input Test Mass
End Test Mass
Signal Recycling Mirror
Photodiode
otod ode
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